Slow steady gyroscope precession

ID: slow-steady-gyroscope-precession

Model the assembly as a heavy symmetric top with a fixed frictionless support, a uniform gravitational field, and centre of mass on its symmetry axis. Assume constant spin, negligible damping, and initial conditions prepared for uniform precession of a heavy symmetric top. Large spin means the transverse angular momentum from precession is small: . Also require . A large spin rate alone does not select steady motion after an arbitrary release.
For an original illustrative calculation, stipulate
The transverse principal moments of inertia are about the pivot, including the parallel axis theorem contribution. These inputs give
The ratio is small; the more direct angular momentum ratio is small too. These are model calculations, not experimental results.
Check the approximation against the existing exact uniform precession of a heavy symmetric top condition. Its total angular momentum is
At constant , differentiating this expression and equating it to the gravitational torque gives
For the slow solution can be evaluated without subtracting two nearly equal numbers:
It exceeds by about . The other solution is about and violates the assumed slow precession; the quadratic's two roots must not be conflated. Its discriminant must be nonnegative for these steady solutions to exist.
Figure 1.
Synthetic steady-precession calculations: larger spin slows the drift and larger transverse torque speeds it up
. Details.
The original curves hold fixed and vary spin and the imposed torque coefficient in . For gravity alone, ; the other curves are hypothetical changes in the transverse torque, not observations of this wheel. Solid curves use the slow quadratic root; dashed curves use . The second panel displays their relative difference. Increasing spin improves this approximation for the parameters shown. It does not remove nutation caused by inappropriate initial conditions.

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